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Bp 300

Manufactured by Bio-Logic
Sourced in Germany

The BP-300 is a benchtop centrifuge designed for general laboratory applications. It features a brushless motor and can achieve a maximum speed of 3,000 RPM. The unit has a rotor capacity of 6 x 15mL tubes and is suitable for a variety of common sample separation tasks.

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5 protocols using bp 300

1

Redox Flow Battery Optimization

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All RFB and SFB measurements were carried out in a custom modified N2 flush box (Terra Universal) with continuous N2 purging. 5.0 mL solution of 0.2 M BTMAP-Fc and 5.0 mL solution of 0.2 M BTMAP-Vi, both with 1.0 M NaCl as the supporting salt, were used as anolyte and catholyte, respectively. Both BTMAP-Fc and BTMAP-Vi were purchased from the Tokyo Chemical Industry Co., Ltd. and used directly. The NMe-TEMPO was synthesized following a previous report50 (link). The electrolyte flow rate was set from 20 to 120 mL min−1 for RFB measurements. Galvanostatic cycling tests were carried out using a Bio-Logic BP-300 potentiostat at desired constant current densities with 0.3 and 1.1 V as the bottom and top potential limits, respectively. A 10 s rest period at open-circuit voltage was employed between each half cycle. The potentiostatic capacity of the RFB was determined by galvanostatic charging/discharging followed by a potential hold at cut-off potentials until the current density reached 1 mA cm−2.
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2

Integrated Solar-Flow Battery Cycling

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Totally, 5.0 mL solution of BTMAP-Vi/Fc with concentrations of 0.1 and 0.2 M in 1.0 M NaCl, or 5.0 mL solution of BTMAP-Fc/ NMe-TEMPO with concentrations of 0.1 M in 1.0 M NaCl were used as the catholyte/anolyte. The electrolyte flow rate was controlled at 40, 60, and 80 mL min1 for the SFB cycling tests. A dual-channel Bio-Logic BP-300 potentiostat was used for the SFB cycling tests. To characterize the charging–discharging behaviors of the integrated SFB device, one potentiostat channel (CH1) was configured as the RFB mode to monitor the potential between the two carbon felt electrodes; the other potentiostat channel (CH2) was configured as solar recharge mode to monitor the charging photocurrent (Fig. 1c).
During the solar charging process, the GaAs photoelectrode was illuminated by one Sun simulation (as described in the PEC characterization section) without applying external bias. A 1.35 h time limit was used to control the SOC below ca. 54%. During the discharging process, the illumination was blocked by a beam shutter, and a discharging current intensity of 11 mA was applied by CH1 until the cell potential reached 0.3 V. The dual-channel potentiostat and the beam shutter of the solar simulator were synchronized and controlled by CH1 and a custom-made electronic control box to enable automated long-term SFB cycling measurements.
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3

Characterization of Materials Using Spectroscopy

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UV–vis absorption spectra
were collected using an Ocean Optics UV–vis spectrometer with
a DH-2000 BAL dual source (deuterium and tungsten) and OCEAN-FX-XRI-ES
diode array detector. Electrochemical measurements were recorded on
either a Biologic SP 300 or Biologic BP 300 potentiostat. FTIR spectra
were collected using a Bruker Alpha FT-IR spectrometer with a Pt-diamond
single-bounce ATR cell and a DTGS detector.
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4

Electrochemical Analysis of Oxygen Evolution

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For the electrochemical analysis, 5 µL of the hydrogel precursor solution was dropped on a rotating glassy carbon (GC) electrode with a working area of 0.196 cm2. The OER experiments were performed in a three-electrode system controlled by a BioLogic BP-300 potentiostat/impedance meter in an O2-saturated 0.1 M KOH electrolyte (Titripur®, Merc, Germany). The rotating ring disk electrode (RRDE-3A) was used at 1600 rpm; GC and Hg/HgO were the working electrode and the reference electrode, respectively. Linear sweep voltammetry (LSV) data was recorded from 1.1 to 2.0 V vs RHE with a 10 mV/s scan rate. The charge transfer resistance (Rct) was determined based on EIS measurements. The spectra were obtained in the frequency range from 10 kHz to 0.1 Hz at 1.7 V vs RHE, and with an amplitude of 10 mV. All potential values were converted to the RHE and then iR-corrected. Cycling voltammetry scans were performed at scan rates of 10, 20, 40, 60, 80, and 100 mV·s−1 to estimate the double-layer capacitance. The non-faradaic potential region was applied (from 1 V to 1.7 V vs RHE).
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5

GaAs Photovoltaic Cell Performance

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Solid-state JV performance of the GaAs cells was measured in a two-electrode configuration63 (link). The LSV measurements were carried out using a Bio-Logic SP-200 potentiostat with a scan rate of 100 mV s−1 under AM 1.5 G one Sun (100 mW cm−2) illumination by a Newport Model 91191 Xenon arc lamp solar simulator. The illumination intensity of the solar simulator was calibrated by a Si photodiode (Thorlabs) before LSV measurements.
The PEC characteristics of the GaAs photoanode were measured using the integrated SFB device under solar cell mode in an N2 flush box by a Bio-Logic BP-300 potentiostat in a two-electrode configuration under one Sun illumination. The LSV measurements were performed with a scan rate of 100 mV s−1. The simulated solar illumination was provided by a Newport Model 67011 quartz tungsten halogen (QTH) solar simulator and guided by a branched flexible silica light guild (Taiopto Mems International Co., Ltd.) fed through an N2 flush box. The QTH solar simulator was calibrated by the same Si photodiode calibration cell to generate the same value of current intensity as that measured under one Sun AM1.5 G illumination by the Newport 91191 simulator.
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